Q.The number density of free electrons in a copper conductor estimated in Example 3.1 is 8.5×1028 m−3. How long does an electron take to drift from one end of a wire 3.0 m long to its other end? The area of cross-section of the wire is 2.0×10−6 m2 and it is carrying a current of 3.0 A.
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🔒 Start your 14-day free trial to unlock the full solution →Concept understanding — Drift Velocity
Drift Velocity: The Slow March of Electrons
Electrons in a metal are always moving — but randomly. At room temperature they zip around at roughly 106 m/s, colliding with the lattice ions every few trillionths of a second. Without an electric field this motion cancels out: for every electron heading left another heads right, so the net velocity is zero.
Apply a battery and the field gives every electron a tiny, steady push in one direction. Between collisions the electron accelerates only briefly before smashing into an ion and losing its directed motion. What survives is a very small average velocity along the field — the drift velocity.
The random thermal speed is about 105 m/s, but the drift velocity is only about 10−4 m/s — about a billion times slower. An electron drifts slower than a snail, yet a lamp lights instantly, because the electric field (not the electrons) propagates at nearly the speed of light and starts every electron drifting almost at once.
The precise definition
Drift velocity (vd) is the average velocity acquired by the charge carriers in a conductor under an applied electric field:
vd=meEτ
where:
- e = electron charge (1.6×10−19 C)
- E = electric field inside the conductor (V/m)
- τ = average relaxation time — the mean time between collisions (s)
- m = electron mass (9.1×10−31 kg)
vd=meEτ
Linking to current
Drift velocity connects the microscopic motion of electrons to the current an ammeter reads:
I=neAvd
where n is the free-electron number density and A the cross-sectional area. A larger vd means more current, but vd stays tiny because τ is tiny (about 10−14 s in copper).
For a copper wire carrying 1 A with area 1 mm² and n≈8.5×1028 m−3:
vd=neAI≈(8.5×1028)(1.6×10−19)(10−6)1≈7×10−5 m/s …
Why this formula?
Drift Velocity: Why the Formula Holds
Let's build this from first principles — understanding why electrons drift the way they do, not just memorizing the formula.
1. The Core Idea: What is Drift Velocity?
In a conductor, free electrons are constantly moving randomly (thermal motion, speeds ~105 m/s). Without an electric field, their net displacement is zero — they're like a swarm of bees buzzing in all directions.
When we apply an electric field E, it gently nudges each electron in the opposite direction (since electrons are negatively charged). This small, steady net velocity superimposed on the random motion is drift velocity (vd).
Key insight: Drift velocity is not the speed of individual electrons — it's the average velocity of the entire electron cloud.
2. The Derivation: Step by Step
Step 1: Force on a single electron
An electron of charge −e in an electric field E experiences:
F=−eE
The magnitude of acceleration (opposite to E) is:
a=mF=meE
where m is the electron's mass.
Step 2: What happens between collisions?
Electrons don't accelerate forever — they keep colliding with atoms/ions in the metal lattice. Let the average time between collisions be τ (relaxation time). Just after a collision an electron's velocity is essentially random (zero average in the field direction); it then accelerates for time τ before the next collision.
Step 3: Drift velocity
Averaging the field-driven velocity over the relaxation time τ gives the net drift:
vd=meEτ
Here τ is the average time since the last collision, so this expression already averages over electrons at every stage between collisions — it is the standard result used in the NCERT treatment.
3. Connecting to Current: The Big Picture
Drift velocity directly gives us current density J:
J=nevd
where n = number of free electrons per unit volume. …
Concept: Drift Velocity — relates current to the average velocity of charge carriers: vd=neAI.
Given I=3.0A, n=8.5×1028m−3, e=1.6×10−19C, A=2.0×10−6m2, L=3.0m:
vd=(8.5×1028)(1.6×10−19)(2.0×10−6)3.0=2.72×1043.0≈1.10×10−4m/s …
Using vd=I/(neA), the drift speed is vd≈1.10×10−4m/s, so the time to drift the 3.0m wire is t=L/vd≈2.72×104s, which is about 7.6 hours.
Why drift velocity is the key
A current is carried by the net drift of free electrons superimposed on their much faster random thermal motion. The relation linking current to that drift speed is
I=neAvd⇒vd=neAI.
Once vd is known, the time to cross the wire's length L is simply t=L/vd.
vd=neAI,t=vdL
Step-by-step solution
1. Known quantities
- n=8.5×1028m−3
- L=3.0m
- A=2.0×10−6m2
- I=3.0A
- e=1.6×10−19C
2. Drift velocity
vd=neAI=(8.5×1028)(1.6×10−19)(2.0×10−6)3.0
Computing the denominator: ne=(8.5×1028)(1.6×10−19)=1.36×1010C/m3, and neA=(1.36×1010)(2.0×10−6)=2.72×104C/(m\cdots). So
vd=2.72×1043.0≈1.10×10−4m/s.
Check units: [n][e][A][vd]=m−3⋅C⋅m2⋅m/s=C/s=A, matching I — confirming the formula is dimensionally consistent.
3. Drift time …
Method: Drift Velocity Formula
This problem uses the drift velocity relation that connects current, charge carrier density, cross-sectional area, and drift speed.
Step-by-step solution
Step 1: Recall the formula for current in terms of drift velocity
The current I in a conductor is given by:
I=neAvd
where:
- n = number density of free electrons (8.5×1028 m−3)
- e = charge of an electron (1.6×10−19 C)
- A = cross-sectional area (2.0×10−6 m2)
- vd = drift velocity of electrons
Step 2: Solve for drift velocity vd
Rearranging:
vd=neAI
Substitute the values:
vd=(8.5×1028)(1.6×10−19)(2.0×10−6)3.0
vd=2.72×1043.0
vd=1.10×10−4 m/s
Step 3: Find the time to drift the given length
Time t is distance divided by drift velocity:
t=vdL=1.10×10−43.0
t=2.72×104 s …
Common Mistakes Students Make on Drift Velocity Problems
Mistake 1: Confusing Drift Speed with Actual Electron Speed
The error: Students often think electrons zoom through wires at near light speed. They calculate a tiny drift velocity and panic, thinking something is wrong.
Why it happens: The signal speed (≈ 3×108 m/s) is confused with drift speed (≈ 10−4 m/s). Electrons actually drift very slowly — like a snail's pace — but the electric field propagates almost instantly.
How to avoid: Remember:
- Drift velocity (vd) = net average velocity of electrons under an electric field
- Signal speed = speed at which current starts flowing (near light speed)
- A slow drift velocity is correct — expect answers in mm/s or μm/s
Mistake 2: Using Wrong Formula or Misplacing Variables
The error: Students write I=neAvd but solve for the wrong quantity, or forget that n is number density (not number of electrons).
Correct formula:
I=neAvd
where:
- I = current (A)
- n = number density (m−3)
- e = charge of electron (1.6×10−19 C)
- A = cross-sectional area (m2)
- vd = drift velocity (m/s)
How to avoid: Write the formula before plugging numbers. Solve for vd explicitly:
vd=neAI
Mistake 3: Forgetting to Convert Units
The error: Using area in cm2 or length in km without converting to SI units.
Example: 2.0×10−6 m2 is already in SI — but if given as 2.0 mm2, students forget 1 mm2=10−6 m2.
How to avoid: Always convert to metres, seconds, amperes before calculation. Write units beside every number.
Mistake 4: Stopping at Drift Velocity Instead of Finding Time
The error: The question asks: "How long does an electron take to drift from one end to the other?" Students calculate vd and stop.
What's needed: After finding vd, use:
t=vdL
where L=3.0 m.
How to avoid: Read the question twice. Underline what is being asked — here it's time, not velocity.
Mistake 5: Arithmetic Errors with Powers of 10
The error: Mismanaging exponents when dividing:
vd=(8.5×1028)(1.6×10−19)(2.0×10−6)3.0
Students often add/subtract exponents incorrectly. …
- GUJCET 2026Set x1 markMCQQ.On increasing the temperature of a conductor, for free electrons ______ increases. (A) drift velocity (B) mobility (C) relaxation time (D) thermal speed
›Reveal solutionSolution
[!TLDR]
Balance condition 62=12X gives X=4Ω — option (B).
Concept
A Wheatstone bridge is balanced (no galvanometer current) when the ratio of resistances in the two arms on one side equals that on the other: QP=SR.
Solution
Taking the four arms in order as P=2Ω, Q=6Ω, R=X, S=12Ω: …
- GUJCET 2025Set 031 markMCQQ.The drift velocity of an electron is vd in a conductor of area of cross-section A and carries a current I. Now, the area of cross-section and current flowing through the conductor are double, then new drift velocity of the electron is ______. (A) 2vd (B) 4vd (C) 4vd (D) vd
›Reveal solutionSolution
Drift velocity vd=neAI, so vd∝AI.
Doubling both current and area: vd′=ne(2A)2I=neAI=vd. The …
- GUJCET 2024Set 131 markMCQQ.The SI units of the current density is ________. (A) Am−2 (B) Am−1 (C) Am−1 (D) Am2
›Reveal solutionSolution
[!TLDR]
J=I/A has units of ampere per square metre, Am−2 — option (A).
Concept
Current density is the electric current per unit cross-sectional area through which it flows: J=AI. Current is in amperes (A) and area in square metres (m2).
Solution …
- GUJCET 2024Set 131 markMCQQ.The magnitude of the drift velocity per unit electric field is known as ________. (A) Charge density (B) Conductivity (C) Mobility (D) Resistivity
›Reveal solutionSolution
Mobility μ is defined as the drift velocity per unit electric field, μ=vd/E.
Concept. In a conductor, vd=μE, so μ=Evd — the magnitude of drift velocity per unit field. …
- GSEB Higher Secondary Certificate (HSC) Examination 2023Set ANNUAL1 markMCQQ.Loop rule of Kirchhoff's is a reflection of ___.(a) Law of conservation of momentum(b) Ohm's law(c) Law of conservation of charge(d) Law of conservation of energy
›Reveal solutionSolution
The loop rule (sum of emf and IR drops around a loop = 0) expresses conservation of energy for a charge carried once around the loop.
Kirchhoff's loop (second) rule: the algebraic sum of changes in potential around any closed loop is zero.
…
- GSEB Higher Secondary Certificate (HSC) Examination 2023Set ANNUAL1 markMCQQ.The colour bands of a carbon resistor with three bands having minimum value are ___ in order.(a) black, brown, silver(b) black, black, silver(c) black, brown, red(d) black, brown, gold
›Reveal solutionSolution
To minimise the value, use the smallest digits and smallest multiplier: black (0), brown (1), silver (x0.01), giving 0.01 ohm - the minimum meaningful three-band value.
Colour code: first two bands are digits, third is the multiplier. Black = 0, brown = 1, silver = x10^-2.
Reading black-brown-silver: digits 0 and 1 give 01 = 1, multiplier 10^-2:
R = 1 x 10^-2 = 0.01 ohm.
…
- GSEB Higher Secondary Certificate (HSC) Examination 2023Set ANNUAL1 markMCQQ.A steady current flows in a metallic conductor of non uniform cross-section, which of following quantities is constant along the conductor?(a) electric field(b) current density(c) current(d) drift speed
›Reveal solutionSolution
Charge conservation in steady state forces the current I to be the same at every cross-section; only I is constant, while J, v_d and E change where the area changes.
In steady state no charge accumulates anywhere, so the same current I passes through every cross-section of the conductor (charge conservation).
…
- GUJCET 2022Set 171 markMCQQ.The number density of free electrons in a copper conductor estimated 8.5×1028 m−3. How long does an electron take to drift from one end of a wire 6 m long to its other end? The area of cross-section of the wire is 1.0×10−6 m2 and it is carrying a current of 1.5 A. (A) 8.1×104 s (B) 5.4×104 s (C) 12.7×104 s (D) 4.5×104 s
›Reveal solutionSolution
Drift speed vd=nAeI≈1.1×10−4 m/s, so the drift time t=vdL≈5.4×104 s.
Concept: Drift velocity vd=nAeI:
vd=(8.5×1028)(1.0×10−6)(1.6×10−19)1.5≈1.1×10−4 m/s …
- GUJCET 2021Set 151 markMCQQ.As following figure 2A current passing through a conducting wire, radius of cross-sectional of wire at point A is 3r and point B is r respectively. Then find the ratio of drift velocity at point A & B. [FIGURE: a tapered (conical) conductor, wide end A of radius 3r, narrow end B of radius r, current I = 2A flowing A to B] (A) 31 (B) 3 (C) 91 (D) 9
›Reveal solutionSolution
Same current, so drift velocity varies inversely with cross-sectional area.
Concept: I=neAvd is constant along the wire, so vd∝A1∝r21. …
- GSEB Higher Secondary Certificate (HSC) Examination 2018Set ANNUAL1 markMCQQ.A wire is uniformly stretched to make its area of cross section (1/n) times (n > 0). What will be its new resistance?(a) n^2 times(b) 1/n^2 times(c) 1/n times(d) n times
›Reveal solutionSolution
Stretching conserves volume; if area becomes A/n the length becomes nL, and since R proportional to L/A the resistance becomes n^2 times the original.
Resistance R = rho L / A. Volume V = L A stays constant during stretching.
…
- GSEB Higher Secondary Certificate (HSC) Examination 2018Set ANNUAL1 markMCQQ.If the current in an electric bulb increases by 2%, what will be the change in the power of a bulb? (Assume that the resistance of the filament of a bulb remains constant).(a) decreases by 2%(b) decreases by 4%(c) increases by 2%(d) increases by 4%
›Reveal solutionSolution
With R fixed, P = I^2 R, so delta_P/P = 2 delta_I/I = 2 x 2% = 4% (an increase).
Power dissipated with constant resistance: P = I^2 R.
Taking the fractional change (differentiate/log): delta_P/P = 2 (delta_I/I).
…
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